Hydrodynamics Optimizing Methods and Tools Part 12 potx

Hydrodynamics – Optimizing Methods and Tools 318 303 313 323 333 343 353 0 100 200 300 400 500 Feed temperature, T F [K] Permeate flux, J [dm 3 /m 2 d] vertical orthogonal Fig. 7. Influence the position of MD module (vertical or orthogonal) on the permeate flux in the case, when inert gas is accumulated inside the module shell The problem of inert gases can be solved in a simple way when an additional port-valve is added to the upper part of housing of vertically positioned module (Fig, 8). It enables the removal of inert gases accumulated in the shell of the module. This prevents a decline of the permeate flux and the module efficiency was progressively increased along with increase of feed temperature (Fig. 9). Similarly as before (Fig. 5), the permeate flux for the counter- current flow was only slightly larger than that obtained for the co-current flow. For this reason, it is advantageous to eliminate gas accumulation in the module channels using co- current flow (Gryta, 2005b). In this case the MD module is vertically positioned, and the streams of feed and distillate flows upwards in the module. This allows to remove the bubbles of inert gases formed from MD module in a natural way. GAS FEED DISTILLATE Fig. 8. The design of module head enables to remove inert gas from module shell The Influence of the Hydrodynamic Conditions on the Performance of Membrane Distillation 319 - counter-current - co-current T D = 293 K 320 325 330 335 340 345 100 200 300 400 500 Permeate flux, J [dm 3 /m 2 d] Feed temperature, T F [K] Fig. 9. Influence the feed temperature and direction of streams flow inside the MD module on the permeate flux 2.3 Hydrodynamic entrance length The distance from the channel inlet to the point of the stabilization of laminar velocity profile is defined as the hydrodynamic entrance length (marked as “L H ”) (Andersson & Irgens, 1990; Chu-Lien et al., 2010; Doughty & Perkins, 1970; Zhang et al., 2010). Different correlations for the calculation of the Nusselt number are presented in literature for entrance and fully developed flow regions (Gryta et al., 1997, 1998). In the membrane systems often the laminar flow is applied. The membrane modules are relatively short; therefore, the flow development in the entrance region cannot be sometimes omitted. It will be suitable only in the case, when the ratio of the entrance region to the total membrane area is low. Heat and mass transfer in membrane-formed parallel-plates channels play a key role for performance analysis and system design. The streams flow in the plate-and-frame module is similar to laminar flow inside the rectangular channel. Therefore, the calculation of L H entrance length can be made based on the Navier-Stokes equations (Bennett & Myers, 1962; Zhang et al., 2010). For the symmetric channels the growing of hydrodynamic boundary layer is completed when the axial line of duct is reached. The solution of Navier-Stokes equations for the flow between the parallel walls is given by Howarth, and for this case we have (Bennett & Myers, 1962): L H =0.015 Re h (9) where h is a high of channel. A similar relation for analysis of flow inside the broad rectangular channel was obtained, but the coefficient value was 0.04 (Prandtl, 1949). The correlation allowing to calculate the L H value for the flow in tubes have a similar form to that presented by equation (9). Most frequently the value of this coefficient is given as equal to 0.03 or 0.0575, whereas the Re number is determined for an average flow rate in the tube. The permeate flow through the porous wall influenced on the velocity profile, however, for most membrane processes (wall Re <1) the analytical solution is sufficient because the symmetric radical of velocity profiles exists. Hydrodynamics – Optimizing Methods and Tools 320 Parallel-plates channels are the most common structure for plate-and-frame modules. They are simple, and easy to assemble. In plate-and-frame modules usually occur a number of smaller parallel channels instead of one wide channel (Gryta et al., 1997). This caused, that the interaction of side walls also have the influence on the formation of velocity profile. The studies carried out to determine the L H value for a channel with width 45 mm and height respectively: 5, 10 and 15 mm gave different results in a comparison with those calculated from Eq.(9). The velocity parabolic profile in XY plane (flow only between parallel plates) was formed earlier, and the observed side–walls effect increases with increasing L H values. Due to the side-walls interactions, the hydrodynamic entrance length was established faster, and indicated nonlinear function (Fig. 10). In the rectangular channel the created temporary parabolic profile (plane XY) was transformed into the deformed parabolic profile (plane XYZ). 0 0.004 0.008 0.012 0.016 0 0.02 0.04 0.06 0.08 0.10 channel height [m]: - 0.005 - 0.010 - 0.015 Flow rate, v [m/s] Hyd. entrance length, L H [m] Fig. 10. Variation of hydrodynamic entrance length with flow rate (profile formed in XY plane). Lines – calculated from Eq. (9) described the flow between parallel plates. According to the theory of boundary layer, the entrance length L H is dependent as follows: L H =f(v A , , a, h) (10) where a is the channel width, v A and are average flow rate and kinematic viscosity, respectively. Taking into consideration a non-linear form of function and the dimensional analysis, the expected function can be expressed as: b2 Hh a L=b1 Re d h (11) where d h is hydraulic diameter. The b1 and b2 coefficients were estimated from the Levenberg-Marquardt Method with minimization of sum of the square deviation. Two hundred of measuring points were used for this analysis. The Snedecors test (F) for significations correlation study has been applied (Volle, 1969). The significance of coefficients study was carried out using Student test (t). In the both tests the signification level has been taken as =0.05. The obtained function was as: 0.5 Hh a L = 0.069 Re d h (12) The Influence of the Hydrodynamic Conditions on the Performance of Membrane Distillation 321 The calculated values of squared coefficient of variation for this equation was 0.95. The results presented in Fig.11 indicated, that the correlation between experimental and calculated data is very good. This confirmed the usefulness of proposed Eq. (12) to calculate the hydrodynamic entrance length under a laminar flow inside the rectangular channel. An estimation of L H values gives possibility to calculate the area of entrance region for the plate and frame modules (Zhang et al., 2010). 0 0.004 0.008 0.012 0.016 0 0.02 0.04 0.06 0.08 0.10 0.12 channel height [m]: - 0.005 - 0.010 - 0.015 Hyd. entrance length, L H [m] Flow rate, v [m/s] Fig. 11. Variation of hydrodynamic entrance length with velocity for water flow inside rectangular channel (velocity profile formed in XYZ plane). Lines – calculated from Eq. (12) 3. Membrane modules for MD process The availability of the industrial MD modules is currently one of the limitations for MD process implementation. Flat-sheet membranes in plate-and-frame modules or spiral wound modules and capillary membranes in tubular modules have been used in various MD studies (Gryta et al, 2000; Schneider et al., 1988). The design of the MD modules should provide not only good flow conditions, but also has to improve the heat transfer and thermal stability (Teoh et al., 2008; Srisurichan et al., 2006; Phattaranawik et al., 2003). 3.1 Capillary MD modules The capillary membrane module is a bundle of porous capillaries packed into a shell similar in configuration to a tube-and-shell heat exchanger (Ju-Meng et al., 2004; Schneider et al., 1988). Because of their very high rate of mass transfer, the capillary modules have been used in many practical applications, such as liquid/liquid extraction, artificial kidney, and desalination studies (Singh, 2006). As a thermally driven process, MD can be significantly affected by temperature polarization (Alklaibi & Lior, 2005; El-Bourawi et al., 2006, Su et al., 2010). Among various types of membrane modules, the capillary module shows the least temperature polarization, so it must have a great future in this field (Zhongwei et al., 2003). In a capillary module used in MD process, the fluid temperatures and transmembrane flux may vary axially alongside the module (Gryta, 2002b). Usually, the feed flows inside the capillary lumen, and distillate flows on the shell side. Theoretically, the capillaries in a bundle can be packed regularly across the shell of a module as in tube-and-shell heat Hydrodynamics – Optimizing Methods and Tools 322 exchanger. In most industrial modules, however, the distribution of capillary is far more arbitrary; the capillaries are randomly packed in the shell. This leads to a range of duct sizes and shapes in the shell, or the module shows a certain extent variation of the local packing fraction (Gryta et al., 2000, Ju-Meng et al., 2004; Zhongwei et al., 2003). The vast majority of the MD processes occur in the regions with the local packing fraction, φ between 0.3 and 0.6. Production rate (93%) of the module is from these regions, and they occupy only 75% of the overall membrane area of the module. In the regions with φ larger than 0.6, the distillate flow rates are too much smaller than that of the feed, so their temperatures are very close to that of the feed. This means that more than 20% of the feed stream goes through the module almost without any driving force for MD process, so the associated membrane area, more than 20% of the total, is ineffective (Ju-Meng et al., 2004). A dislocation of the membranes can be limited using a high value of packing fraction φ. However, this caused a reduction of the channel dimensions on the shell side and the increase in the flow resistance, which hinders the application of appropriate high flow rate of distillate. This is an important aspect, because when the distillate flow rate increases, its temperature will become less affected by heat transfer and vapor condensation from the feed side of the membrane, and so does the feed stream. This means that the increment of flow rates can enlarge the temperature difference between these two streams in the module, and in this way the MD process is improved (Zhongwei et al., 2003). With regards to this, a value of the φ coefficient in MD modules should amount to 0.4-0.6 (Gryta et al., 2000; Ju-Meng et al., 2004; Schneider et al., 1988). In order to limit the changes of capillaries arrangement inside the shell, one should use such assembly of capillaries, which prevents their free displacements. Good results have been obtained by assembling the membrane capillaries inside the sieve baffles or by a tight packing of membranes in a form of braided capillaries (Gryta et al., 2000; Schneider et al., 1988). A comparison of results obtained for the module having the same value of φ coefficient equal to 0.33, but differing in the manner of membranes assembling is presented in Fig. 12. A traditional construction (module M1) based upon the fixation of a bundle of parallel membranes solely at their ends 330 340 350 360 370 0 100 200 300 400 500 module: - M1 - M2 - M3 Permeate flux, J [dm 3 /m 2 d] Feed temperature, T F [K] Fig. 12. The influence of feed temperature and the mode of membrane arrangement in a capillary module on the permeate flux. M1 - bundle of parallel membranes; M2 - braided capillaries; and M3 – capillaries mounted inside mesh of sieve baffles The Influence of the Hydrodynamic Conditions on the Performance of Membrane Distillation 323 results in that the membranes arrange themselves in a random way. This creates the unfavorable conditions of cooling of the membrane surface by the distillate, which resulted in a decrease of the module efficiency (Gryta et al., 2000; Schneider et al., 1988; Zhongwei et al., 2003). In module M3 the membranes were positioned in every second mesh of six sieve baffles, arranged across the housing with in 0.1–0.15 m. The most advantageous operating conditions of MD module were obtained with the membranes arranged in a form of braided capillaries (module M2). This membrane arrangement improves the hydrodynamic conditions (shape of braided membranes acted as a static mixer), and as a consequence, the module yield was enhanced (Gryta et al., 2000) A good indicator of the hydrodynamic conditions in a module is the analysis of residence time distribution (RTD). The value of liquid flowing time through the module with good design solution should be closed to the RTD value. The effect of shell-side residence time distribution on mass transfer performance was studied (Lemanski & Lipscomb, 1995). It was pointed out that plug flow would be obtained in an ideal hollow fiber module, but in real shell-side flow the distribution of fluid across the capillary bundle tended to broaden the RTD. The studies of residence time distribution for a colored impulse in the modules M1-M3 were shown in Figs. 13-14. The RTD value was calculated for assumed plug flow, taking into account a value of φ=0.34. A dye injected into the module appeared the fastest at the outlet of module in the case of module M1 (bundle of parallel capillaries), moreover, the residence time of dye in this module was also the longest. Such result indicates that the non- uniform distribution of capillaries inside the shell caused the formation of channels with different diameters. The distillate was flowing faster in wider channels than the calculated average velocity. As a result, colored water was out flowing faster from the module exit than the calculated RTD value. 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.6 0.7 0.8 0.9 1.0 Flow rate, v [m/s] module: - M1 - M2 - M3 Relative time, t/t RTD Fig. 13. The influence of flow rate on the relative initial time of colour water residence inside the module. M1 - bundle of parallel membranes; M2 - braided capillaries; and M3 – capillaries mounted inside mesh of sieve baffles Hydrodynamics – Optimizing Methods and Tools 324 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 1.0 1.2 1.4 1.6 1.8 2.0 2.2 -M1 -M2 -M3 Flow rate, v [m/s] Relative time, t/t RTD Fig. 14. The influence of flow rate on the total time of dye residence inside the module. M1 - bundle of parallel membranes; M2 - braided capillaries; and M3 – capillaries mounted inside mesh of sieve baffles As a result of larger values of local capillary packing, the water flows slower in the narrow channels (larger resistance of flow), what prolonged the residence time of dye in the module. An increase in the flow rate increases the turbulence of water flow in the module and dye was washing out faster also from the narrow channels. Due to, the residence time of liquid in the module for larger velocities was closer to the average value. The housings of modules M1-M3 were made of glass tube. This enables the observation of dye spreading out inside their interior. The visual observations of colored streams confirmed these conclusions. The time of water flow in the two remaining modules (M2 and M3) was definitely closer to the RDT value. This indicates, that the dimensions of channels between the capillary membranes had the similar dimension and liquid flows uniformly through the module cross-section. The visual observations also confirmed this fact; dye was uniformly filling up the housing space. The situation was different in the case of module M1, where due to differences in the flow rates, preceded diversity in the intensity of water coloration. A prolongation of residence time of dye in the module was observed at the flow rates higher than 0.5 m/s. This was associated with growing intensity of liquid mixing in their internal. It was observed, that the vortexes appeared along with the increase in the flow rates. As a result, the portion of colored water were backward transferred, what caused the coloration of new portion of water and due to growing volume of colored water, an apparent longer time of residence in the module was noticed. 3.2 Module with flat sheets membranes The flat sheet membranes are used in the plate-and-frame modules and spiral-wound module design. In the first case, the flat sheet membranes are assembled between the plates having several channels. The membranes are stacked in flow channels connected in series or in parallel. Usually, the plates are rectangular with the flow from one end to the other. The spiral-wound module uses the flat sheet membranes wound around a central tube. The membranes are glued along three sides to form “leaves” A feed channel spacer (a net-like sheet) is placed between the leaves to define the channel height. A three-channel design can be used in the spiral wound module, which allows the recovery of heat transferred from the feed to distillate (Fig.15). The Influence of the Hydrodynamic Conditions on the Performance of Membrane Distillation 325 feed 273 K distillate retentate 300 K 346 K 353 K external heat source MD module heat Fig. 15. Module channel arrangement for permeate gap membrane distillation (Winter et al., 2011) Based on this solution, spiral wound MD modules with a 5-14 m 2 effective membrane area have been developed by Fraunhofer Institute for Solar Energy System (Winter et al., 2011). The cold feed water enters the condenser channel and is heated to approximately 346 K due to internal heat recovery. An external heat source (e.g. solar collector) heats the feed water up to 353 K. The hot feed flows through the evaporator channel in a counter-current direction and exits the module at 300 K. Water vapour passes through the membrane and condenses in the distillate channel. The latent and sensible heat is transferred through the condenser foil to preheat the feed water in the condenser channel. Due to increasing flow resistance, a fast feed flow cannot be used in such a module. As a result, decreasing the vapour pressure with salinity reduces the process driving force. The feed water salinity is considered one of the most important parameters affecting the spiral wound module concept. Larger flow velocities can be used in the plate-and-frame module than in the spiral wound modules. Therefore, the plate-and-frame modules can be utilized for the separation of concentrated salt solutions. The channels in the plate-and-frame modules are shorter; and as a result, an excessive increase of hydraulic pressure is limited. For this reason, several authors suggest the use of spacers as the turbulence promoters (Chu-Lien et al., 2010, Martínez & Rodríguez-Maroto, 2006), because turbulent flow is an appropriate method to decrease the negative effect of polarization phenomena. The turbulent or upper transition flow regime was found in the spacer-filled channels for UF although the Reynolds numbers were still in the laminar regime (Phattaranawik et al., 2003). Net-type spacers are often put into the flow channels in the membrane processes to improve the mass transfer and to reduce the effect of concentration polarization and fouling. The spacers can also be utilized in MD since they destabilize the flow and create eddy currents in the laminar regime so that heat, and mass transfer are enhanced (Teoh et al., 2008; Phattaranawik et al., 2003). The permeate fluxes obtained from the experiments with spacer-filled channels were compared with those obtained in the experiments performed under laminar and turbulent flow conditions, but for modules with non-filled channels. In the case of experiments with the spacers, a 26–56% increase in the permeate fluxes was achieved, compared with the fluxes performed under laminar flow (Martínez & Rodríguez-Maroto, 2006). However, these fluxes were much lower than those obtained from turbulent flow conditions in the empty channels. This results from the fact, that the feed evaporates during the flow through a module, causing a relatively fast decrease of the feed temperature, which reduces a value of driving force for mass transfer. Thus, in the MD process both the value of the flow rate (m/s) and the volumetric flow (m 3 /s of feed per unit of the membrane area) have a considerable importance. A sufficiently large value of heat transfer coefficient (e.g. 5000 W/m 2 K) allowing to eliminate the temperature polarization, can be generated for laminar Hydrodynamics – Optimizing Methods and Tools 326 flow (Gryta, 2002b). Although a further increase in the flow rate will not have a substantial influence on the reduction of the temperature polarization, the value of volumetric flow (m 3 /s m 2 ) will increase significantly, and beneficial results, such as enhancement of the permeate flux, will be obtained. The nets exhibit the filtration properties, which hinder the use of modules with the channels filled with the nets in certain applications (Fig.16). Fig. 16. SEM image of deposit formed inside the net supporting the membrane in the MD module The concentration of non-clarified juices cannot be carried out with the utilization of such modules (Jiao et al., 2004). The desalination process of hard water, in which significant amounts of CaCO 3 precipitates are formed (Gryta, 2005a, 2006b), can be another negative exemplary. As demonstrated the nets, favors the hydrogenous crystallization (Gryta, 2009), which would increases the intensity of scaling in the module. The flat sheet membranes exhibit a low resistance to mechanical damage; therefore, they are reinforced by the application of supporting nets. However, the presence of nets decreases the heat and mass transfer to membrane surfaces, while significantly enhancing the polarization phenomena. These phenomena reduce the difference between T 1 and T 2 interfacial temperatures (Fig. 1), compared to the design when no net was used. Consequently, the driving force for mass transfer is also reduced in the case of net supported membranes. Therefore, a module design in which a part of channel is empty, while a part is filled by net supporting the membrane, significantly influenced reduction of MD efficiency (Gryta et al., 1997). The module performance can be improved by elimination of nets and by an increase of the number of channels on a module plate so that their walls fill the role of edges supporting the membrane (Fig. 17). It was found that an arrangement of edges every 15-20 mm was appropriate for the membranes made of PVDF and PTFE with the thickness of 100-150 m (Gryta et al., 1997; Tomaszewska et al., 2000). [...]... rougher and heterogeneous surface; the hydrate shell seems to become loosely, and easily collapsed by the buoyant motion of target gas trapped in the shell (a) Elapsed time (b) Elapsed time Fig 7 CHClF2 hydrate formation in water (a) and 400ppm SDS aqueous solution (b) at 0.40MPa, 283K (Tajima et al., 2010b) 346 Hydrodynamics – Optimizing Methods and Tools 14 2 10 8 8 aK*x10 [mol /(s·J)] 12 6 4 2... one at QL = 0 Despite holding 344 Hydrodynamics – Optimizing Methods and Tools thermodynamic conditions (operation pressure and temperature) constant for each gas, the gas hydrate formation is accelerated Hydrate slurry formation is observed for both water flow conditions even though the hydrate shell formation is observed at QL = 0 Without respect to gas species and hydrate structure, the water flow... in Fig 19 Fig 18 The schema of water flow inside the distribution channel of the plate -and- frame module presented in Fig 17 328 Hydrodynamics – Optimizing Methods and Tools Fig 19 A visualization of feed flow in the distribution channel 3.2.1 Uniformity of flow In the capillary modules good conditions of mixing and a flow close to plug flow can be achieved by using an appropriate design, e.g by assembling... & Fane, A.G (2005) Humic acid fouling in the membrane distillation, Desalination, Vol.174, No.1, (April 2005), pp 63–72, ISSN 0011-9164 334 Hydrodynamics – Optimizing Methods and Tools Srisurichan, S.; Jiraratananon, R & Fane, A.G (2006) Mass transfer mechanisms and transport resistances in direct contact membrane distillation process, Journal of Membrane Science, Vol.277, No.1-2, (June 2006), pp 186–194,... gas hydrate formation have been demonstrated, including a spray (Fukumoto et al., 2001) or jet reactor (Szymcek et al., 2008; Warzinski et al., 2008), and a bubble column (Luo et al, 2007; Hashemi et al., 2009) 336 Hydrodynamics – Optimizing Methods and Tools besides general stirred tank However, gas hydrate formation is very complicated by the presence of three phases (gas-liquid-solid) during gas hydrate... the reactor The injected gas is converted to gas hydrate in the static mixer unit and unconverted gas is vented from at the top of the reactor Transport of formed hydrate particles are carried out with the water fluid, and the hydrate particles are settled and separated at the recovery vessel Water without large hydrate particle, therefore, is always supplied to the reactor The recovery vessel is set... formation patterns in the semi-batch flow reactor Conditions (a) and (b) are gas-water system, (c) and (d) are time-course in the hydrate formation, hydrate slurry and hydrate plug (Tajima et al., 2007) 342 Hydrodynamics – Optimizing Methods and Tools 8 278±0.4K 280±0.4K 281±0.4K 282±0.4K 4 7 aK* [10 mol /(s·J)] 2 3 -8 -8 2 aK* [10 mol /(s·J)] 5 2 1 0 CHClF2 0 0.1 0.2 6 5 4 3 2 1 0.3 0.4 0.5 Pressure [MPa]... distance of ¼ plate width from each end of the channel The module was A) feeding 0.1 dm3/min B) feeding 0.21 dm3/min 330 Hydrodynamics – Optimizing Methods and Tools C) feeding 0.44 dm3/min D) feeding 0.86 dm3/min Fig 21 Visualization of variations in the flow rates of water (302 K) in the particular channels of the module (channel dimension 10x3.5 mm) with a two-point feeding of module plate feeding with... improvement in direct contact membrane distillation Desalination, Vol.253, (April 2010), pp 16–21, ISSN 0011-9164 332 Hydrodynamics – Optimizing Methods and Tools Criscuoli, A.; Carnevale, M.C & Drioli, E (2008) Evaluation of energy requirements in membrane distillation, Chemical Engineering and Processing, Vol.47, No.7, (July 2008), pp 1098-1105, ISSN 0009-2509 Drioli, E.; Curcio, E.; Criscuoli, A & Di... temperature, gas and water flow rates, gas species, and so on The relation between the hydrate formation pattern and these conditions will be discussed again later 3 Hydrate formation rate analysis There are many discussion about gas hydrate formation kinetics With regard as this point, another book about natural gas hydate is available (Sloan and Koh, 2008) Although gas hydrate nucleation and growth processes . Hydrodynamics – Optimizing Methods and Tools 320 Parallel-plates channels are the most common structure for plate -and- frame modules. They are simple, and easy to assemble. In plate -and- frame. bundle can be packed regularly across the shell of a module as in tube -and- shell heat Hydrodynamics – Optimizing Methods and Tools 322 exchanger. In most industrial modules, however, the distribution. parallel membranes; M2 - braided capillaries; and M3 – capillaries mounted inside mesh of sieve baffles Hydrodynamics – Optimizing Methods and Tools 324 0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 1.0 1.2 1.4 1.6 1.8 2.0 2.2 -M1